JPS62123788A - Variable wavelength type laser oscillator - Google Patents

Variable wavelength type laser oscillator

Info

Publication number
JPS62123788A
JPS62123788A JP26301385A JP26301385A JPS62123788A JP S62123788 A JPS62123788 A JP S62123788A JP 26301385 A JP26301385 A JP 26301385A JP 26301385 A JP26301385 A JP 26301385A JP S62123788 A JPS62123788 A JP S62123788A
Authority
JP
Japan
Prior art keywords
wavelength
laser
concave mirror
laser beam
light
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Pending
Application number
JP26301385A
Other languages
Japanese (ja)
Inventor
Naoto Nishida
直人 西田
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Toshiba Corp
Original Assignee
Toshiba Corp
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Toshiba Corp filed Critical Toshiba Corp
Priority to JP26301385A priority Critical patent/JPS62123788A/en
Publication of JPS62123788A publication Critical patent/JPS62123788A/en
Pending legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01SDEVICES USING THE PROCESS OF LIGHT AMPLIFICATION BY STIMULATED EMISSION OF RADIATION [LASER] TO AMPLIFY OR GENERATE LIGHT; DEVICES USING STIMULATED EMISSION OF ELECTROMAGNETIC RADIATION IN WAVE RANGES OTHER THAN OPTICAL
    • H01S3/00Lasers, i.e. devices using stimulated emission of electromagnetic radiation in the infrared, visible or ultraviolet wave range
    • H01S3/05Construction or shape of optical resonators; Accommodation of active medium therein; Shape of active medium
    • H01S3/08Construction or shape of optical resonators or components thereof
    • H01S3/081Construction or shape of optical resonators or components thereof comprising three or more reflectors
    • H01S3/0811Construction or shape of optical resonators or components thereof comprising three or more reflectors incorporating a dispersive element, e.g. a prism for wavelength selection

Landscapes

  • Physics & Mathematics (AREA)
  • Electromagnetism (AREA)
  • Engineering & Computer Science (AREA)
  • Plasma & Fusion (AREA)
  • Optics & Photonics (AREA)
  • Lasers (AREA)

Abstract

PURPOSE:To eliminate an injection laser oscillator and an optical system by a method wherein a wavelength selecting element is provided outside the concave mirror of an unstable resonator and a laser beam with a required wavelength is selectively reflected by the wavelength selecting element and injected into the unstable resonator. CONSTITUTION:When a laser medium 11 starts oscillation, a natural emitted light with a low output intensity and a wide wavelength range is introduced to a prism 6, which is a wavelength selecting element, through the light transmitting part 13b of a concave mirror 13. Only the wavelength component of the natural emitted light which enters vertically to a reflective surface 6a returns into an unstable resonator through the light transmitting part 13b of the concave mirror 13 along the same light path as the incident path and an initial laser oscillation is created between a convex mirror 12 and the prism 6. The light emitted by this oscillation is a single wavelength laser beam and is resonated and amplified between the convex mirror 12 and the concave mirror 13 without changing its spectral properties and outputted from the non-coated part 12b of the convex mirror 12 as a laser beam of high output.

Description

【発明の詳細な説明】 〔発明の技術分野〕 本発明は、波長の異なるレーザ光を選択的に発振出力可
能な波長可変形レーザ発振装置の改良に関する。
DETAILED DESCRIPTION OF THE INVENTION [Technical Field of the Invention] The present invention relates to an improvement in a wavelength tunable laser oscillation device capable of selectively oscillating and outputting laser beams having different wavelengths.

〔発明の技術的背景〕[Technical background of the invention]

従来、この種の装置の一つとしてインジェクション・ロ
ッキング方式を用いたものが知られている。第3図(a
>はこのインジェクション・ロッキング方式を適用した
し〜ザ発振装置の構成を示すもので、この装置は広帯域
発振特性を有するレーザ媒質1の両端側にそれぞれ対向
面に高反射コーティング2a、3aを施した凸面鏡2お
よび凹面鏡3を配設してこれらにより不安定共振器を構
成し、かつ低出力の注入用レーザ発振器4を設けて、こ
のレーザ発振器4から出力されたレーザ光を光学系5を
介して上記凹面鏡2の光軸上に設けた透光部3bから上
記不安定共振器内に注入し、これにより不安定共振器の
発振波長を上記注入用レーザ光の波長にロックしてこの
ロックされた波長の発振レーザ光を上記凸面鏡2の無反
射コーティング部2bから高出力で送出するようにしだ
ものである。尚、第3図(b)は発振出力レーザ光のビ
ームパターンを示すものである。このような装置であれ
ば、広帯域にエネルギが分散されたレーザ媒質1のレー
ザ光のうち所望の波長のみを選択的に高出力で発振出力
することができ、非常に有用である。
Conventionally, one using an injection locking method is known as one of this type of devices. Figure 3 (a
> shows the configuration of a laser oscillation device to which this injection locking method is applied, and this device has high reflection coatings 2a and 3a applied to opposite ends of a laser medium 1 having broadband oscillation characteristics, respectively. A convex mirror 2 and a concave mirror 3 are arranged to form an unstable resonator, and a low-output injection laser oscillator 4 is provided, and the laser beam output from the laser oscillator 4 is transmitted through an optical system 5. The injection is carried out into the unstable resonator through the transparent part 3b provided on the optical axis of the concave mirror 2, thereby locking the oscillation wavelength of the unstable resonator to the wavelength of the injection laser beam. The oscillation laser beam having the same wavelength is transmitted from the non-reflection coating portion 2b of the convex mirror 2 at high output. Incidentally, FIG. 3(b) shows a beam pattern of the oscillation output laser light. Such a device is very useful because it can selectively emit only a desired wavelength of laser light from the laser medium 1 with energy dispersed over a wide band at a high output.

C背景技術の問題点〕 ところが、このような従来の波長可変形レーザ発振装置
は、インジェクション・ロッキングを起こさせるために
注入用レーザ発振器4を設けなければならず、またその
注入レーザ光を不安定共振器に導入する光学系5を必要
とするため、構成が複雑で大形化し、これにより装置が
極めて高価になる欠点があった。
C. Problems of Background Art] However, in such a conventional wavelength tunable laser oscillator, an injection laser oscillator 4 must be provided to cause injection locking, and the injection laser beam may become unstable. Since the optical system 5 is required to be introduced into the resonator, the structure is complicated and large, which has the drawback of making the device extremely expensive.

〔発明の目的〕[Purpose of the invention]

本発明は、注入用レーザ発振器や光学系等の大掛りな構
成要素を不要とし、これにより構成が簡単かつ小形で安
価にて高出力の狭帯域レーザ光を得ることができる波長
可変形レーザ発振装置を提供することを目的とする。
The present invention eliminates the need for large-scale components such as an injection laser oscillator and optical system, and thereby enables a wavelength tunable laser oscillation that is simple, compact, and inexpensive to obtain high-output narrowband laser light. The purpose is to provide equipment.

〔発明の概要〕[Summary of the invention]

本発明は、上記目的を達成するために、不安定共振器の
凹面鏡の外側に波長選択素子を配設し、この波長選択素
子により、不安定共振器から上記凹面鏡の光軸上に設け
た透光部を経て導出されるレーザ光のうち、所望の波長
のレーザ光を選択的に反射して上記凹面鏡の透光部を介
して不安定共振器内に注入することにより、不安定共振
器に所望波長のロッキングを起こさせるようにしたもの
である。
In order to achieve the above object, the present invention disposes a wavelength selection element outside the concave mirror of the unstable resonator, and uses this wavelength selection element to move the unstable resonator from the optical axis of the concave mirror. Of the laser light emitted through the optical part, laser light of a desired wavelength is selectively reflected and injected into the unstable resonator through the transparent part of the concave mirror. This is designed to cause locking of a desired wavelength.

〔発明の実施例〕[Embodiments of the invention]

第1図(a)は、本発明の一実施例における波長可変形
レーザ発振装置の構成を示すもので、11は広帯域発振
特性を有するレーザ媒質を示している。このレーザ媒質
11の両端側にはそれぞれ不安定共振器を構成する凸面
鏡12および凹面鏡13が配設されている。これらの凸
面鏡12および凹面鏡13はそれぞれ互いに対向するレ
ーザ反射面に高反射コーティングを施したものである。
FIG. 1(a) shows the configuration of a wavelength tunable laser oscillation device according to an embodiment of the present invention, and numeral 11 indicates a laser medium having broadband oscillation characteristics. A convex mirror 12 and a concave mirror 13, which constitute an unstable resonator, are disposed at both ends of the laser medium 11, respectively. These convex mirror 12 and concave mirror 13 each have a high reflection coating applied to their mutually opposing laser reflecting surfaces.

また凸面[12のレーザ反射面のうち外周部分には無反
射コーティング12bが施されており、この部分から発
振レーザ光が出力される。また凹面鏡13の光軸部分に
は所定径の透光部13bが設けてあり、この透光部13
bからレーザ注入が行なわれるようになっている。
Further, an anti-reflection coating 12b is applied to the outer peripheral portion of the laser reflecting surface of the convex surface [12], and the oscillated laser beam is output from this portion. Further, a light transmitting portion 13b having a predetermined diameter is provided at the optical axis portion of the concave mirror 13.
Laser injection is performed from b.

さて、上記凹面鏡13の外側の光軸上には波長選択素子
としてのプリズム6が配設しである。このプリズム6は
、波長選択面6bとこの波長選択面6bを経て入射され
たレーザ光を反射する反射面とを億えたもので、この反
射面には高反射コーティング6aが施されている。尚、
この反射面は凹面に形成されており、その曲率は前記凸
面鏡12の反射面の曲率とこの反射面からプリズム6の
波長選択面6bまでの光路長とにより設定される。また
プリズム6は、図示しない角度調整機構により矢印へ方
向に揺動可能に支持されており、この揺動によりレーザ
光の反射角を可変可能となっている。
Now, on the optical axis outside the concave mirror 13, a prism 6 as a wavelength selection element is arranged. The prism 6 includes a wavelength selection surface 6b and a reflection surface that reflects the laser beam incident through the wavelength selection surface 6b, and this reflection surface is coated with a high reflection coating 6a. still,
This reflective surface is formed into a concave surface, and its curvature is set by the curvature of the reflective surface of the convex mirror 12 and the optical path length from this reflective surface to the wavelength selection surface 6b of the prism 6. Further, the prism 6 is supported so as to be swingable in the direction of the arrow by an angle adjustment mechanism (not shown), and this swinging allows the reflection angle of the laser beam to be varied.

この様な構成であるから、レーザ媒質11が発振を開始
すると、低出力で波長幅の広い自然放出光が凹面鏡13
の透光部13k)を経てプリズム6に導かれる。そうす
ると、上記広波長幅の自然放出光7は例えば第2図に示
す如くプリズム6の波長選択面6bで波長毎に異なる屈
折率で屈折されてプリズム6内に入射され、しかるのち
反射面6aで反射されて上記凹面鏡13へ戻る。このと
き、上記各波長の自然放出光のうち上記反射面6aに垂
直に入射した波長成分の自然放出光7aのみが入射経路
と同じ経路を経て凹面鏡13の透光部13aから不安定
共振器内に戻り、しかるのち凸面鏡12と上記プリズム
6の反射面6aとの間で共振作用により波長が選択され
た初期レーザ発振が生じる。この結果不安定共振器は、
外部の注入用レーザ発振器から単一波長のレーザ光を注
入された場合と等価となり、これにより上記プリズム6
から入射されたレーザ光に発振波長がロックされて、こ
の波長のレーザ光のみがそのスペクトル的性質を可変す
ることなく凸面鏡12および凹面鏡13間で共振増幅さ
れ、高出力のレーザ光として凸面鏡12の無コーテイン
グ部12bから出力される。第1図(b)はその出力レ
ーザ光のビームパターンを示すものである。ちなみに、
上記レーザ光の出力エネルギは、例えば同等制限を設け
ずに広帯域発振させたときに460〜soonm(波長
幅40nm)で出力エネルギが50m Jのレーザ光が
得られるXeF(C−+A)レーザをレーザ媒質として
用いた場合で、波長幅が0.5nlllで出力エネルギ
が50〜60m Jの狭帯域レーザ光を得られる。
With such a configuration, when the laser medium 11 starts oscillating, spontaneously emitted light with low output and a wide wavelength range is transmitted to the concave mirror 13.
The light is guided to the prism 6 through the transparent portion 13k). Then, as shown in FIG. 2, for example, the spontaneously emitted light 7 with a wide wavelength width is refracted by the wavelength selection surface 6b of the prism 6 with a different refractive index for each wavelength, and then enters the prism 6, and then is reflected by the reflection surface 6a. It is reflected and returns to the concave mirror 13. At this time, among the spontaneously emitted light of each wavelength, only the spontaneously emitted light 7a of the wavelength component that is perpendicularly incident on the reflective surface 6a passes through the same path as the incident path from the transparent part 13a of the concave mirror 13 into the unstable resonator. Then, initial laser oscillation with a selected wavelength occurs due to resonance between the convex mirror 12 and the reflective surface 6a of the prism 6. As a result, the unstable resonator is
This is equivalent to injecting a single wavelength laser beam from an external injection laser oscillator, and this causes the prism 6 to
The oscillation wavelength is locked to the laser beam incident from the laser beam, and only the laser beam of this wavelength is resonantly amplified between the convex mirror 12 and the concave mirror 13 without changing its spectral properties, and is emitted from the convex mirror 12 as a high-power laser beam. It is output from the non-coating section 12b. FIG. 1(b) shows the beam pattern of the output laser light. By the way,
The output energy of the above laser beam is, for example, an XeF (C-+A) laser that can obtain a laser beam of 50 mJ at 460 to soon m (wavelength width 40 nm) when oscillated in a wide band without setting equivalent restrictions. When used as a medium, a narrow band laser beam with a wavelength width of 0.5 nllll and an output energy of 50 to 60 mJ can be obtained.

このように本実施例であれば、不安定共振器と波長選択
素子としてのプリズム6とを組合わせたことにより、注
入用レーザ発振器を使用する場合と全く同様に所望波長
の高出力のレーザ光を発生させることができ、しかも従
来の様に注入用レーザ発振器やその注入用光学系を全く
用いることなく、極めて簡単な構成で実現することがで
き、この結果小形で安価な装置を提供することができる
In this way, in this embodiment, by combining the unstable resonator and the prism 6 as a wavelength selection element, a high-output laser beam with a desired wavelength can be generated, just like when using an injection laser oscillator. can be generated, and can be realized with an extremely simple configuration without using an injection laser oscillator or an injection optical system as in the past, and as a result, a small and inexpensive device can be provided. I can do it.

また、本実施例ではプリズム6を角度調整機構で支持し
て反射角度を可変設定できるように構成しであるので、
この角度調整機構によりプリズムの反射角を適宜調整す
るだけで、簡単に所望の波長のレーザ光を得ることがで
きる。
Furthermore, in this embodiment, the prism 6 is supported by an angle adjustment mechanism so that the reflection angle can be variably set.
Laser light of a desired wavelength can be easily obtained by simply adjusting the reflection angle of the prism appropriately using this angle adjustment mechanism.

尚、本発明は上記実施例に限定されるものではない。例
えば、波長選択素子としてはプリズム以外にグレーティ
ングを用いてもよい。その他、不安定共振器の構成や広
帯域発振特性を有するレーザ媒質の種類、波長選択素子
の構成等についても、本発明の要旨を逸脱しない範囲で
種々変形して実施できる。
Note that the present invention is not limited to the above embodiments. For example, instead of a prism, a grating may be used as the wavelength selection element. In addition, various modifications may be made to the configuration of the unstable resonator, the type of laser medium having broadband oscillation characteristics, the configuration of the wavelength selection element, etc. without departing from the gist of the present invention.

〔発明の効果〕〔Effect of the invention〕

以上詳述したように本発明によれば、不安定共振器の凹
面鏡の外側に波長選択素子を配設し、この波長選択素子
により、不安定共振器から上記凹面鏡の光軸上に設けた
透光部を経て導出されるレーザ光のうち、所望の波長の
レーザ光を選択的に反射して上記凹面鏡の透光部を介し
て不安定共振器内に注入することにより、不安定共振器
に所望波長のロッキングを起こさせるようにしたことに
よって、注入用レーザ発振器や光学系等の大掛りな構成
要素を不要にすることができ、これにより構成が簡単か
つ小形で安価にて高出力の狭帯域し一ザ光を得ることが
できる波長可変形レーザ発振装置を提供することができ
る。
As described in detail above, according to the present invention, a wavelength selection element is disposed outside the concave mirror of the unstable resonator, and the wavelength selection element allows the unstable resonator to be connected to the transparent mirror provided on the optical axis of the concave mirror. Of the laser light emitted through the optical part, laser light of a desired wavelength is selectively reflected and injected into the unstable resonator through the transparent part of the concave mirror. By causing locking of the desired wavelength, large-scale components such as an injection laser oscillator and an optical system can be eliminated. It is possible to provide a wavelength tunable laser oscillation device that can obtain a single laser beam over a wide range of wavelengths.

【図面の簡単な説明】[Brief explanation of drawings]

第1図(a)、(b)および第2図は本発明の一実施例
における波長可変形レーザ発振装置を説明するためのも
ので、第1図(a)は同装置の構成を示す図、第1図(
b)は出力レーザ光のビームパターンを示す図、第2図
はプリズムの動作を説明するための拡大図、第3図(a
)、(b)は従来の波長可変形レーザ発振装置を説明す
るためのもので、(a>は同装置の構成を示す図、(b
)は出力レーザ光のビームパターンを示す図である。 11・・・広帯域発振特性を有するレーザ媒質、12・
・・凸面鏡、12a・・・高反射コーティング部、12
b・・・無反射コーティング部、13・・・凹面鏡、1
3a・・・高反射コーティング部、13b・・・透光部
、6・・・プリズム、6a・・・反射面、6b・・・波
長選択面、7・・・レーザ光。 出願人代理人 弁理士 鈴江武彦 (a)               (b)第1図 第2図 第3図
FIGS. 1(a), (b), and 2 are for explaining a wavelength tunable laser oscillation device according to an embodiment of the present invention, and FIG. 1(a) is a diagram showing the configuration of the device. , Figure 1 (
b) is a diagram showing the beam pattern of the output laser beam, FIG. 2 is an enlarged diagram for explaining the operation of the prism, and FIG.
) and (b) are for explaining a conventional wavelength tunable laser oscillation device, (a> is a diagram showing the configuration of the device, and (b) is a diagram showing the configuration of the device.
) is a diagram showing a beam pattern of output laser light. 11... Laser medium having broadband oscillation characteristics, 12...
...Convex mirror, 12a...High reflection coating part, 12
b... Anti-reflection coating part, 13... Concave mirror, 1
3a... High reflection coating part, 13b... Transparent part, 6... Prism, 6a... Reflective surface, 6b... Wavelength selection surface, 7... Laser light. Applicant's agent Patent attorney Takehiko Suzue (a) (b) Figure 1 Figure 2 Figure 3

Claims (2)

【特許請求の範囲】[Claims] (1)広帯域のレーザ光を発振するレーザ媒質と、この
レーザ媒質の一端側に配置されたレーザ出力部を有する
凸面鏡と、光軸上に透光部を有し前記レーザ媒質の他端
側に配置されて前記凸面鏡とともに不安定共振器を構成
する凹面鏡と、この凹面鏡の外側に配置され凹面鏡の前
記透光部から導出されたレーザ光のうち所望波長のレー
ザ光を選択して前記透光部を介して不安定共振器内に注
入する波長選択素子とを具備したことを特徴とする波長
可変形レーザ発振装置。
(1) A laser medium that oscillates a broadband laser beam, a convex mirror having a laser output section disposed on one end of the laser medium, and a convex mirror having a light-transmitting section on the optical axis and disposed on the other end of the laser medium. A concave mirror arranged to form an unstable resonator together with the convex mirror and a laser beam of a desired wavelength guided from the light-transmitting part of the concave mirror arranged outside the concave mirror are selected, and a laser beam of a desired wavelength is selected from the light-transmitting part. What is claimed is: 1. A wavelength tunable laser oscillation device comprising: a wavelength selection element for injecting into an unstable resonator through a wavelength selection element.
(2)波長選択素子は、選択レーザ光の反射面を有する
プリズムからなり、上記反射面による反射角度が可変可
能に構成されたものである特許請求の範囲第(1)項記
載の波長可変形レーザ発振装置。
(2) The wavelength-tunable type according to claim (1), wherein the wavelength selection element is composed of a prism having a reflective surface for the selective laser beam, and the reflection angle by the reflective surface is variable. Laser oscillation device.
JP26301385A 1985-11-22 1985-11-22 Variable wavelength type laser oscillator Pending JPS62123788A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP26301385A JPS62123788A (en) 1985-11-22 1985-11-22 Variable wavelength type laser oscillator

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP26301385A JPS62123788A (en) 1985-11-22 1985-11-22 Variable wavelength type laser oscillator

Publications (1)

Publication Number Publication Date
JPS62123788A true JPS62123788A (en) 1987-06-05

Family

ID=17383673

Family Applications (1)

Application Number Title Priority Date Filing Date
JP26301385A Pending JPS62123788A (en) 1985-11-22 1985-11-22 Variable wavelength type laser oscillator

Country Status (1)

Country Link
JP (1) JPS62123788A (en)

Cited By (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH01207983A (en) * 1988-02-16 1989-08-21 Mitsubishi Electric Corp Solid laser equipment
JPH01270372A (en) * 1988-04-22 1989-10-27 Mitsubishi Electric Corp laser equipment
JPH022188A (en) * 1988-06-13 1990-01-08 Shimadzu Corp excimer laser equipment
WO1996031929A1 (en) * 1995-04-03 1996-10-10 Komatsu Ltd. Narrow-band laser
CN104300352A (en) * 2014-10-16 2015-01-21 北京工业大学 Light pulse repetition rate spectrum spreader
JP2015525002A (en) * 2012-08-16 2015-08-27 インテグレイテッド オプティックス,ウーアーベー Method for generating or amplifying multiple wavelengths of laser radiation in a single optical resonator

Cited By (7)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH01207983A (en) * 1988-02-16 1989-08-21 Mitsubishi Electric Corp Solid laser equipment
JPH01270372A (en) * 1988-04-22 1989-10-27 Mitsubishi Electric Corp laser equipment
JPH022188A (en) * 1988-06-13 1990-01-08 Shimadzu Corp excimer laser equipment
WO1996031929A1 (en) * 1995-04-03 1996-10-10 Komatsu Ltd. Narrow-band laser
US6101211A (en) * 1995-04-03 2000-08-08 Komatsu, Ltd. Narrow-band laser apparatus
JP2015525002A (en) * 2012-08-16 2015-08-27 インテグレイテッド オプティックス,ウーアーベー Method for generating or amplifying multiple wavelengths of laser radiation in a single optical resonator
CN104300352A (en) * 2014-10-16 2015-01-21 北京工业大学 Light pulse repetition rate spectrum spreader

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